There is a discussion in [1]} that the ERG evolution cannot really be trusted for \(t \gtrsim 1\) . However, we see now that the smallest \(|M_1^2|\)  at \(t=0.27\)  is a thousand times greater than the cut-off \(\Lambda ^2\)  that was assumed to exist in the theory. At every other values of \(t\)  we see in Fig. REF  that \(M_1^2\)  exceeds \(\Lambda ^2\)  even more. And in the small \(t\)  limit which is most interesting for us the masses become infinitely many times greater than \(\Lambda \) .
